Chapter 10: Q1P (page 438)
Show that the differential equations for V and A (Eqs. 10.4 and 10.5) can be written in the more symmetrical form
Where
Short Answer
The differential equations for V and Ain the symmetrical form are derived as
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Chapter 10: Q1P (page 438)
Show that the differential equations for V and A (Eqs. 10.4 and 10.5) can be written in the more symmetrical form
Where
The differential equations for V and Ain the symmetrical form are derived as
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(a) Find the fields, and the charge and current distributions, corresponding to
(b) Use the gauge function to transform the potentials, and comment on the result.
A particle of charge q is traveling at constant speed v along the x axis. Calculate the total power passing through the plane X, at the moment the particle itself is at the origin. [ Answer ]
Question: Suppose you take a plastic ring of radius and glue charge on it, so that the line charge density is . Then you spin the loop about its axis at an angular velocity . Find the (exact) scalar and vector potentials at the center of the ring. [Answer:]
For the configuration in Ex. 10.1, consider a rectangular box of length , width , and height , situated a distanced above the plane (Fig. 10.2).
Figure 10.2
(a) Find the energy in the box at time, and at.
(b) Find the Poynting vector, and determine the energy per unit time flowing into the box during the interval.
(c) Integrate the result in (b) from to , and confirm that the increase in energy (part (a)) equals the net influx.
A particle of chargeq moves in a circle of radius a at constant angular velocity . (Assume that the circle lies in thexy plane, centered at the origin, and at time the charge is at role="math" localid="1653885001176" , on the positive x axis.) Find the Li茅nard-Wiechert potentials for points on the z-axis.
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